JPS6034318B2 - image spatial frequency analyzer - Google Patents
image spatial frequency analyzerInfo
- Publication number
- JPS6034318B2 JPS6034318B2 JP16657280A JP16657280A JPS6034318B2 JP S6034318 B2 JPS6034318 B2 JP S6034318B2 JP 16657280 A JP16657280 A JP 16657280A JP 16657280 A JP16657280 A JP 16657280A JP S6034318 B2 JPS6034318 B2 JP S6034318B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- image
- video signal
- output
- spatial frequency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000003287 optical effect Effects 0.000 claims description 20
- 238000001228 spectrum Methods 0.000 claims description 8
- 230000006835 compression Effects 0.000 claims description 6
- 238000007906 compression Methods 0.000 claims description 6
- 238000005070 sampling Methods 0.000 claims description 6
- 239000002131 composite material Substances 0.000 claims description 3
- 238000004364 calculation method Methods 0.000 description 20
- 230000003595 spectral effect Effects 0.000 description 9
- 230000002457 bidirectional effect Effects 0.000 description 8
- 238000010586 diagram Methods 0.000 description 8
- 238000002604 ultrasonography Methods 0.000 description 5
- 238000000034 method Methods 0.000 description 4
- 238000005314 correlation function Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 230000007274 generation of a signal involved in cell-cell signaling Effects 0.000 description 3
- 230000010355 oscillation Effects 0.000 description 3
- 238000000926 separation method Methods 0.000 description 3
- 238000005311 autocorrelation function Methods 0.000 description 2
- 238000010276 construction Methods 0.000 description 2
- 230000000875 corresponding effect Effects 0.000 description 2
- 230000003111 delayed effect Effects 0.000 description 2
- 239000003292 glue Substances 0.000 description 2
- 230000001360 synchronised effect Effects 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000002596 correlated effect Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000010606 normalization Methods 0.000 description 1
- 239000011295 pitch Substances 0.000 description 1
- 230000002250 progressing effect Effects 0.000 description 1
- 238000010183 spectrum analysis Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R23/00—Arrangements for measuring frequencies; Arrangements for analysing frequency spectra
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Measuring Frequencies, Analyzing Spectra (AREA)
- Closed-Circuit Television Systems (AREA)
Description
【発明の詳細な説明】
この発明はテレビ画像における水平走査方向の空間周波
数成分を入力画像に対応した形で画像に構成し、表示す
るようにした画像空間周波数アナライザに関するもので
ある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an image spatial frequency analyzer that configures spatial frequency components in the horizontal scanning direction of a television image into an image in a form corresponding to an input image and displays the image.
従来より、テレビカメラで画像を入力し、電気光学的手
法を用いた空間的実時間相関演算処理を行なって、前記
画像の水平走査方向相関画像を得、これを受像器画面上
に表示する画像相関装置がある。Conventionally, an image is input by a television camera, and a spatial real-time correlation calculation process is performed using an electro-optical method to obtain a horizontal scanning direction correlation image of the image, which is then displayed on the screen of a receiver. There is a correlation device.
このような装置では、相関演算に使用する2つの信号が
共にテレビ画像映像信号等の被演算処理信号であるため
、相関出力画像を検出しても、テレビ画像に含まれる空
間周波数成分の検出は困難である。すなわち、自己相関
出力画像では、入力画像の周期性が検出できるだけであ
り、相互相関出力画像においても特定対象信号に対する
類似度(重なり具合)が測定できるのみである。ここで
筆者等が先に学会(電子通信学会論文誌の197単王3
月Vol.62一A,No.3「超音波光変調器とTV
カメラを用いた画像相関装置の−構成法」)にて発表し
た装置例、すなわち、従来の画像相関装置について構成
法と動作原理を述べる。In such a device, the two signals used in the correlation calculation are both processed signals such as television image video signals, so even if the correlation output image is detected, the spatial frequency components contained in the television image cannot be detected. Have difficulty. That is, in the autocorrelation output image, only the periodicity of the input image can be detected, and in the cross-correlation output image, only the degree of similarity (degree of overlap) with respect to the specific target signal can be measured. Here, the authors first discuss the 197 single king 3 of the journal of the Institute of Electronics and Communication Engineers.
Month Vol. 621A, No. 3 “Ultrasonic light modulator and TV
We will describe the construction method and operating principle of the conventional image correlation device, which is an example of the device presented in "Construction Method of Image Correlation Device Using a Camera").
第4図に従来装置の構成略図を示す。この装置は、一般
に使用されているテレビカメラの映像信号が、電気光学
的相関器に用いられている超音波光変調器への入力信号
として適当な繰返し周期と周波数帯域を持つことに着目
し、前記相関器によって相関処理すべきテレビ画像の各
水平走査ごとの映像出力信号を1次元自己相関演算し、
この相関演算結果を受像器画面上で画像に構成するもの
である。よって出力画像として、入力画像の水平走査方
向自己相関画像を得ることができる。第4図に示した装
置では、自己相関をとるべき入力画像13を双方向婦引
発振器15で発生させた周波数7.87球日2の三角波
で双方向水平走査を行なうテレビカメラ14で撮影し、
得られた複合映像信号を映像信号と水平垂直同期パルス
信号とに分離するため同期パルス分離回路101こ加え
る。FIG. 4 shows a schematic diagram of the configuration of a conventional device. This device focuses on the fact that the video signal of a commonly used television camera has a repetition period and frequency band suitable as an input signal to an ultrasonic optical modulator used in an electro-optic correlator. performing a one-dimensional autocorrelation calculation on the video output signal for each horizontal scan of the television image to be correlated by the correlator;
The results of this correlation calculation are constructed into an image on the screen of the receiver. Therefore, a horizontal scanning direction autocorrelation image of the input image can be obtained as an output image. In the apparatus shown in FIG. 4, an input image 13 to be autocorrelated is captured by a television camera 14 that performs bidirectional horizontal scanning using a triangular wave with a frequency of 7.87 pitches 2 generated by a bidirectional oscillator 15. ,
A synchronization pulse separation circuit 101 is added to separate the obtained composite video signal into a video signal and horizontal and vertical synchronization pulse signals.
ここで分離された映像信号は、後述する光学的相関演算
の条件を満す目的で、映像信号パルス化回路9に送られ
設定閥値との比較により白黒2値を表わす2値パルス映
像信号に変換される。この2値パルス映像信号は一対の
パルス振幅変調可能な正弦波発振器la,lbに外部変
調信号として加えられる。前記発振器は超音波光変調器
5a,5b内に各1枚づつ配置されている超音波振動子
の共振周波数で発振し、発振数は発振器内で前記2値パ
ルス映像信号により振幅変調を受け出力される。この発
振器出力信号は前記超音波振動子に加えられ、超音波光
変調器5a,5b内に空間的超音波信号として放射され
る。次に光学的相関器について説明する。The video signal separated here is sent to the video signal pulsing circuit 9 for the purpose of satisfying the conditions for optical correlation calculation described later, and is converted into a binary pulse video signal representing black and white binary values by comparison with a set threshold value. converted. This binary pulse video signal is applied as an external modulation signal to a pair of sine wave oscillators la and lb which are capable of pulse amplitude modulation. The oscillator oscillates at the resonance frequency of the ultrasonic transducers placed in each of the ultrasonic light modulators 5a and 5b, and the number of oscillations is amplitude modulated by the binary pulse video signal within the oscillator and output. be done. This oscillator output signal is applied to the ultrasound transducer and radiated into the ultrasound light modulators 5a, 5b as spatial ultrasound signals. Next, the optical correlator will be explained.
光学系の光源にはしーザー4を用い、レーザービームを
レンズで拡大した後、前記超音波光変調器5a,5bの
光入射窓に入射させる。一対の前記超音波光変調器5a
,5bは互いに超音波進行方向が逆向きになり、かつ、
超音波進行方向と光軸とが直角に交わるように構成配置
されている。この超音波光変調器5a,5bを通過した
光東は前記変調器内の空間的超音波信号によって部分的
に位相変調を受け、レンズで収束されて焦点面に隆点を
作る。焦点面面は光検出フィル夕6が配置され、超音波
振動子の共振周波数波による1次回折光を通過検出する
。この光検出フィル夕6を通過した光は光電変換器7に
入射し電気信号に変換される。一般に、超音波信号の振
幅が小さな場合振幅値と1次回折光振幅値は比例関係に
あり、また、光振幅値の自乗である光量値に比例する光
電変換器出力電流値は、超音波信号振幅値の自乗に比例
することが知られている。光学的相関演算の原理につい
ては後に詳述する。さて、前記同期パルス分離回路10
にて分離された同期パルスは水平同期時間遅延回路11
に送られ、時間遅れを施された後混合器12に加えられ
る。この混合器12は前記光電変換器7で得られる相関
出力信号に遅延同期パルスを付加して複合映像信号を作
るものであって、混合器出力信号は受像器16において
画像に構成される。前記水平同期時間遅延回路11の遅
延時間をを水平同期時間の約1′2,32ysに定める
ことにより、前記入力画像13の自己相関画像を前記受
像器16の画面の中央に表示することが可能である。次
に光学的相関演算の原理について述べる。A laser beam 4 is used as the light source of the optical system, and after the laser beam is expanded by a lens, it is made incident on the light incidence windows of the ultrasonic light modulators 5a and 5b. A pair of the ultrasonic light modulators 5a
, 5b have opposite directions of ultrasound propagation, and
The ultrasonic wave propagation direction and the optical axis are arranged so as to intersect at right angles. The light beams that have passed through the ultrasonic light modulators 5a and 5b are partially phase modulated by the spatial ultrasonic signals in the modulators, and are converged by a lens to form a ridge on the focal plane. A photodetection filter 6 is disposed on the focal plane, and detects the first-order diffracted light generated by the resonance frequency wave of the ultrasonic transducer. The light that has passed through the photodetection filter 6 enters a photoelectric converter 7 and is converted into an electrical signal. Generally, when the amplitude of the ultrasonic signal is small, the amplitude value and the first-order diffracted light amplitude value are in a proportional relationship, and the photoelectric converter output current value, which is proportional to the light amount value which is the square of the light amplitude value, is the ultrasonic signal amplitude It is known that it is proportional to the square of the value. The principle of optical correlation calculation will be explained in detail later. Now, the synchronous pulse separation circuit 10
The synchronization pulse separated by the horizontal synchronization time delay circuit 11
and is added to the mixer 12 after being subjected to a time delay. This mixer 12 adds a delayed synchronization pulse to the correlation output signal obtained by the photoelectric converter 7 to create a composite video signal, and the mixer output signal is configured into an image in the image receiver 16. By setting the delay time of the horizontal synchronization time delay circuit 11 to approximately 1'2,32 ys of the horizontal synchronization time, it is possible to display the autocorrelation image of the input image 13 at the center of the screen of the image receptor 16. It is. Next, the principle of optical correlation calculation will be described.
概略は双方向水平走査によって得た、各走査ごとに走査
方向が反転している映像信号を、一対の超音波光変調器
5a,5bで空間的に反転・遅延・シフト(移動)させ
、光信号に変換してレンズによる積分演算を行ない、映
像信号中の時間的に隣りあった、すなわちテレビ画面上
では上下の関係にある映像信号間の相互相関関数を自己
相関関数に近似させて得ることである。第5図に示すよ
うに入力画像は2値画像でP(Q,8)とし、垂直同期
パルスより教えてn回目の水平走査で得た映像信号をf
(Q,n)とする。第6図に示すように、2値パルス映
像信号に整形され、f(Q,n)で振幅変調された超音
波信号は超音波光変調器内の超音波振動子に加えられる
。超音波光変調器5a,5bは超音波進行方向が互いに
逆向きになるように配置されているため、超音波光変調
器内の超音波信号はU,(x,n),U2(一×,n)
と書ける。超音波光変調器5aは同5bに比べ超音波進
行方向長さが長く作られており、前記超音波信号U,(
x,n)がレーザー光東内に達する時間は同U2(一×
,n)が同じく達する時間より1水平走査時間63.5
一sだけ遅れる。よって、レーザー光東内で重なる超音
波信号はU,(x,n)とり(一×,n十1)である。
光学系内での2信号の重ね合せは積演算で表わされ、レ
ンズによる収束作用は積分演算で表わされる。また、U
,(x,n),U2(一×,n+1)は超音波速度vで
超音波光変調器内を移動していることを考慮すれば、超
音波信号によって生じた回折光のみを光検出フィル夕6
で検出し、光電変換することによって次に示す相関出力
C(t,i)が電流値とし得られる。‘1}式において
dはしーザー光束の幅を示し、g(x,i)はU(x,
n)の包絡線、すなわち、映像信号f(Q,n)のQを
xに線形変換した関数を表わす。Basically, a video signal obtained by bidirectional horizontal scanning, the scanning direction of which is reversed for each scan, is spatially inverted, delayed, and shifted (moved) by a pair of ultrasonic optical modulators 5a and 5b. To obtain a cross-correlation function between temporally adjacent video signals, that is, a vertical relationship on a TV screen, by approximating the cross-correlation function to an autocorrelation function by converting it into a signal and performing an integral calculation using a lens. It is. As shown in Fig. 5, the input image is a binary image P (Q, 8), and the video signal obtained in the nth horizontal scan after being taught from the vertical synchronization pulse is f
Let it be (Q, n). As shown in FIG. 6, the ultrasonic signal that has been shaped into a binary pulse video signal and amplitude-modulated by f(Q, n) is applied to an ultrasonic transducer in an ultrasonic light modulator. Since the ultrasonic light modulators 5a and 5b are arranged so that the directions of ultrasonic propagation are opposite to each other, the ultrasonic signals in the ultrasonic light modulators are U, (x, n), U2 (1× ,n)
It can be written as The ultrasonic light modulator 5a is made longer in the ultrasonic propagation direction than the ultrasonic light modulator 5b, and the ultrasonic light modulator 5a has a longer length in the ultrasonic propagation direction than the ultrasonic light modulator 5b.
The time it takes for x, n) to reach the laser beam east is U2(1×
, n) reach the same time, one horizontal scanning time is 63.5
There will be a delay of one second. Therefore, the number of ultrasonic signals that overlap within the laser beam is U, (x, n) and (1 x, n + 1).
The superposition of two signals within the optical system is expressed by a product operation, and the convergence effect by a lens is expressed by an integral operation. Also, U
, (x, n), U2 (1 x, n+1) are moving inside the ultrasonic optical modulator at the ultrasonic velocity v, so only the diffracted light generated by the ultrasonic signal is detected by the photodetection filter. Evening 6
By detecting it and photoelectrically converting it, the following correlation output C(t,i) can be obtained as a current value. '1} In the formula, d represents the width of the Caesar luminous flux, and g(x, i) represents U(x,
n), that is, a function obtained by linearly converting Q of the video signal f(Q, n) to x.
テレビカメラの双方向走査回数が画像の大きさに比べて
十分多ければ、g(X,i)芋g(一×,i+1)…■
の関係が成り立ち、‘2)式を{1ー式に代入してを得
る。If the number of bidirectional scans of the TV camera is sufficiently large compared to the size of the image, the following relationship holds true: Assign to and get.
糊式はg(x,i)、すなわちf(Q,i)の自己相関
関数を表わす。C(t,n),f(Q,n)は共に水平
走査回数nにおける関数であるから、C(t,n)をf
(t,n)の同期信号を使用して画像に構成すれば、入
力して2値画像の水平走査方向自己相関画像が得られる
。ただし、糊式を実行して各水平走査映像信号の独立し
た相関出力を得るためには、各映像信号の前後にこれと
等しい長さの無信号部分が必要であることから、入力可
能な映像信号の長さは水平同期時間の1/沙〆下に制限
される。また、光学的相関器では光電変換器7の自乗特
性により、次に示す自乗値相関演算が行なわれる。【4
}式を‘3}式の相関演算と等価にするため、g(x,
n)を〔1,0〕の2値に制限する必要があり、具体的
には入力画像を白黒2値画像に限定するか、映像信号を
閥値回路を用いて2値パルス化している。以上が従来装
置の構成ならびに動作原理の概要である。本発明は以上
に述べた画像相関装置を改良し、相関演算を応用してテ
レビ画像に含まれている空間周波数成分を検出し、画像
の形で表示させることを目的としている。The glue equation represents the autocorrelation function of g(x,i), ie, f(Q,i). Since both C(t, n) and f(Q, n) are functions of the number of horizontal scans n, C(t, n) is
If an image is constructed using a synchronization signal of (t, n), a horizontal scanning autocorrelation image of a binary image can be obtained. However, in order to perform the glue method and obtain independent correlation outputs for each horizontal scanning video signal, a no-signal portion of equal length is required before and after each video signal, so it is necessary to The length of the signal is limited to 1/sa of the horizontal synchronization time. Further, in the optical correlator, the following square value correlation calculation is performed due to the square characteristic of the photoelectric converter 7. [4
} expression is equivalent to the correlation operation of expression '3}, g(x,
It is necessary to limit n) to a binary value of [1, 0], and specifically, the input image is limited to a black and white binary image, or the video signal is converted into a binary pulse using a threshold circuit. The above is an overview of the configuration and operating principle of the conventional device. An object of the present invention is to improve the above-described image correlation device, apply correlation calculations to detect spatial frequency components contained in television images, and display the detected spatial frequency components in the form of images.
すなわち、テレビカメラで得た入力画像の映像信号と、
時間とともに周波数が直線変化する線形FM信号との相
互相関演算を実時間で行ない、この相関出力をブラウン
管面上に掃引して入力画像の水平走査方向空間周波数ス
ペクトル画像を表示することを特徴とした画像空間周波
数アナラィザを提供することにある。この目的を達成す
るため、糠拍FM信号発生装置と、スペクトル画像表示
装置を設け、また、アナログ値映像信号と、線形FM信
号との相互相関演算を実現するため、信号圧縮回路を付
加した。In other words, the video signal of the input image obtained by the television camera,
A cross-correlation calculation with a linear FM signal whose frequency changes linearly with time is performed in real time, and this correlation output is swept onto the cathode ray tube surface to display a horizontal scanning direction spatial frequency spectrum image of the input image. An object of the present invention is to provide an image spatial frequency analyzer. To achieve this purpose, a FM signal generating device and a spectral image display device were provided, and a signal compression circuit was added to realize cross-correlation calculation between the analog value video signal and the linear FM signal.
さらに、映像信号中に無信号部分を形成するための、映
像信号サンプリング回路を設けた。つぎに、この発明を
図面により具体的に説明する。Furthermore, a video signal sampling circuit was provided to form a no-signal portion in the video signal. Next, this invention will be specifically explained with reference to the drawings.
第1図は本発明の画像空間周波数アナラィザの実施例に
おける構成図である。FIG. 1 is a block diagram of an embodiment of the image spatial frequency analyzer of the present invention.
光学的相関器101の相互相関演算動作は従来装置の原
理と同様である。第1図において、単方向または双方向
水平走査を行なうテレビカメラ14によって得られた入
力画像13の映像信号は、水平垂直同期パルスを除去す
ると同時に、各水平走査で得られる映像信号を1つおき
にサンプリングして出力する映像信号サンプリング回路
18に加えられる。また、同時に前記テレビカメラ14
の出力はモニターテレビ17にも送られ、撮影中の入力
画像を表示する。前記映像信号サンプリング回路18の
出力は自乗圧縮回路19に送られ、自乗圧縮をうける。
すなわち、前記自乗圧縮回路19の入力映像信号f(t
)とすれば、同回路出力信号はノf(x)となる。この
信号は、すでに述べた光学的相関器を構成している振幅
変調可能な正弦波発振器laに外部変調信号として加え
られる。次に、線形FM信号の発生装置を説明する。線
形FM信号の周波数を周期的に直線変化させる周波数婦
引用三角波を発生する掃引信号発生回路20の出力は、
周波数変調可能な発振器(周波数変調発振器)21に外
部変調信号として加えられる。前記周波数変調発振器2
1で発生した線形FM信号は、振幅変調可能な正弦波発
振器lbに外部変調信号として加えられる。このとき前
記正弦波発振器lbの発振数が、線形FM信号によって
200%の過変調となるように変調度を設定すれば、線
形FM信号の自乗圧縮信号で前記発振波を振幅変調した
のと同様になる。すなわち、三角関数の性質{■S雲}
2=季(1十のSa) …‘51を考えれば、{5ー
式右辺は100%振幅変調時の外部変調波、同式左辺は
200%過変調時の外部変調波の自乗と考えられる。The cross-correlation calculation operation of the optical correlator 101 is similar to the principle of the conventional device. In FIG. 1, the video signal of an input image 13 obtained by a television camera 14 that performs unidirectional or bidirectional horizontal scanning is removed by removing the horizontal and vertical synchronizing pulses, and at the same time removing every other video signal obtained in each horizontal scanning. The video signal is added to a video signal sampling circuit 18 which samples and outputs the video signal. At the same time, the television camera 14
The output is also sent to a monitor television 17 to display the input image being photographed. The output of the video signal sampling circuit 18 is sent to a square compression circuit 19 and subjected to square compression.
That is, the input video signal f(t
), the output signal of the circuit becomes f(x). This signal is applied as an external modulation signal to the amplitude modulated sinusoidal oscillator la, which constitutes the optical correlator described above. Next, a linear FM signal generator will be explained. The output of the sweep signal generation circuit 20 that generates a frequency triangular wave that periodically and linearly changes the frequency of the linear FM signal is as follows.
It is applied as an external modulation signal to an oscillator capable of frequency modulation (frequency modulation oscillator) 21. The frequency modulation oscillator 2
The linear FM signal generated in step 1 is applied as an external modulation signal to an amplitude modulated sinusoidal oscillator lb. At this time, if the degree of modulation is set so that the number of oscillations of the sine wave oscillator lb is overmodulated by 200% by the linear FM signal, it is equivalent to amplitude modulating the oscillation wave with a square compressed signal of the linear FM signal. become. In other words, the properties of trigonometric functions {■S cloud}
2 = Season (10 Sa)... Considering '51, the right side of the equation 5 is considered to be the external modulation wave at 100% amplitude modulation, and the left side of the same equation is the square of the external modulation wave at 200% overmodulation. .
よって、周波数が2倍となることを除けば、200%過
変調状態を設定することは、自乗圧縮波で外部変調をか
けたことに等しい。さて、この線形FM信号波と前記自
乗圧縮映像信号f(x)との相互相関関数Cs(t,B
)は次式で表わされる。■式8は線形FM信号の繰返し
回数、k‘ま相算の定数、dは光束軸、xは超音波光変
調器内の超音波進行方向軸、Fsは線形FM信号の初期
周波数、Fcは同じく周波数時間変移度を表わす。Therefore, except that the frequency is doubled, setting a 200% overmodulation state is equivalent to applying external modulation with a square compressed wave. Now, the cross-correlation function Cs(t,B
) is expressed by the following formula. ■Formula 8 is the number of repetitions of the linear FM signal, k' is a constant for phase calculation, d is the beam axis, x is the axis of the ultrasound propagation direction in the ultrasonic optical modulator, Fs is the initial frequency of the linear FM signal, and Fc is Similarly, it represents the degree of frequency-time variation.
第2図は‘6}式が相関器内で実現される場合のタイム
チャートを示している。同図aは掃引信号発生回路20
の掃引信号を示し、同図bは前記掃引信号の周期で周波
数変化を繰返し行なう線形FM信号を表わしている。同
図cは1水平走査おきにサンプリングして得た映像信号
であり、図中信号範囲と記した部分に入力画像の映像信
号が含まれている。前記線形FM信号bと同映像信号c
は、おのおの超音波光変調器内を互いに逆方向に速度v
で進行している。よって、この2信号が光東を同時に横
切った部分で相互相関演算が行なわれる。同図dはこの
相互相関演算結果を示している。線形FM信号の周波数
変移度Fcが小さな場合、各映像信号と相関演算を実行
中の光東内の線形FM信号は、一定の周波数をもつ正弦
波信号と見なせる。よって、各映像信号は、おのおの周
波数の異なる正弦波信号と相互相関演算を行なうことに
なり、相関出力の大きさは、映像信号と正弦波信号との
類似度、すなわち、映像信号に含まれる正弦波信号周波
数の成分値を示す。同図cに示すように映像信号中に周
波数fPの信号が含まれている場合、この信号と線形F
M信号の周波数fPの部分が光東d内で重なった時刻t
Pにおいて相関出力振幅値は最大値を示し、波形は2P
の周波数で振動する。この時、図示したように線形FM
信号の初期部分に土d/2の空間距離を有する直流部分
を作成しておけば、線形FM信号の繰返し時刻t=0,
T,2r,・・・では常に映像信号の波形の全面積、す
なわち直流成分が出力される。この値を装置の正規化の
基準値に使用すれば、前述したような周波数fPのみの
信号を有する映像信号の成分値は基準値と等しくなり、
また、種々の成分値が出力される入力画像の場合には、
基準値に対する成分値の割合をもって各周波数成分値と
することができる。次に、前述の相関演算における映像
信号と各周波数正弦波との相関結果は、周波数的に離散
したものであるため、これらを周波数スペクトル画像に
構成する方法を説明する。FIG. 2 shows a time chart when formula '6} is realized within the correlator. Figure a shows the sweep signal generation circuit 20.
Fig. 1b shows a linear FM signal whose frequency changes repeatedly at the period of the sweep signal. Figure c is a video signal obtained by sampling every other horizontal scan, and the video signal of the input image is included in the portion marked as signal range in the figure. The linear FM signal b and the same video signal c
are the velocities v in opposite directions within each ultrasonic light modulator.
It is progressing. Therefore, a cross-correlation calculation is performed at the portion where these two signals cross the light east at the same time. Figure d shows the results of this cross-correlation calculation. When the frequency shift degree Fc of the linear FM signal is small, the linear FM signal in Koto, which is undergoing correlation calculation with each video signal, can be regarded as a sine wave signal with a constant frequency. Therefore, each video signal undergoes a cross-correlation calculation with a sine wave signal having a different frequency, and the magnitude of the correlation output is determined by the degree of similarity between the video signal and the sine wave signal, that is, the sine wave signal included in the video signal. Indicates the component value of the wave signal frequency. As shown in c in the same figure, if the video signal contains a signal with a frequency fP, this signal and the linear F
Time t when the frequency fP part of the M signal overlaps in Koto d
The correlation output amplitude value shows the maximum value at P, and the waveform is 2P
vibrates at the frequency of At this time, as shown in the figure, the linear FM
If a DC part with a spatial distance of d/2 is created in the initial part of the signal, the repetition time t=0,
At T, 2r, . . . , the entire area of the video signal waveform, that is, the DC component, is always output. If this value is used as the standard value for device normalization, the component value of the video signal having only the frequency fP signal as described above will be equal to the standard value,
In addition, in the case of an input image that outputs various component values,
Each frequency component value can be defined as the ratio of the component value to the reference value. Next, since the correlation results between the video signal and each frequency sine wave in the above correlation calculation are discrete in terms of frequency, a method of configuring them into a frequency spectrum image will be described.
第3図はTV画面上の入力画像とその空間周波数スペク
トル画像の構成法を示している。前記スペクトル画像の
成分の大きさは輝度で表現される。1水平走査で得られ
る映像信号の横幅Thは線形FM信号の繰返し周期Tf
に比べ小さいものとすれば、1周期の線形FM信号に対
して多くの映像信号が相関演算を行なう。FIG. 3 shows how to construct an input image on a TV screen and its spatial frequency spectrum image. The magnitude of the component of the spectral image is expressed by brightness. The width Th of the video signal obtained in one horizontal scan is the repetition period Tf of the linear FM signal.
If it is small compared to , many video signals undergo correlation calculations for one cycle of linear FM signal.
よって、スペクトル表示画面上でスペクトル成分を表わ
す輝点を、線形FM信号の周波数掃引信号で左右に掃引
すれば、線形FM信号の種々の周波数帯城における映像
信号との相互相関出力、すなわちスペクトル成分が画面
横方向に表示される。同図に示した例では、入力画像、
スペクトル画像とも双方向水平走査で表示しているが、
これは単一方向水平走査でも良い。さて、スペクトル画
面横方向に表示されるスペクトル成分は、各々の輝点が
入力画像の1つおきの水平走査映像信号中に含まれる周
波数成分値を示している。よって、さらに縄点をテレビ
カメラ14の垂直同期パルスに同期させて画面上を上か
ら下に掃引すれば、同図に示すような水平走査位置に対
応して入出力画像を得る。この麓点で構成されるスペク
トル画像は、線形FM信号の周波数婦引信号とテレビカ
メラ14の垂直掃引信号とで描かれるリサージュ図形と
なるため、前記2信号の繰返し周期を整数倍よりわずか
にずらせることによって細かな網目状となり、出力画面
を均一に覆うことができる。ゆえに、入力画像の水平走
査方向空間スペクトル画像が出力画面上に表示でき、こ
のスペクトル画像は入力画像の変化に応じた実時間表示
画像となる。本発明は以上のような構成であり、テレビ
カメラ14で撮影可能な画像であれば動きのある画像で
あってもスペクトル分析が可能である効果を有する。Therefore, if the bright spots representing the spectral components are swept left and right on the spectrum display screen using the frequency sweep signal of the linear FM signal, the cross-correlation output with the video signal in various frequency bands of the linear FM signal, that is, the spectral components is displayed horizontally on the screen. In the example shown in the figure, the input image,
Both spectral images are displayed using bidirectional horizontal scanning.
This may be a unidirectional horizontal scan. Now, in the spectrum components displayed in the horizontal direction of the spectrum screen, each bright spot indicates a frequency component value included in every other horizontal scanning video signal of the input image. Therefore, if the rope point is further synchronized with the vertical synchronization pulse of the television camera 14 and swept from top to bottom on the screen, an input/output image corresponding to the horizontal scanning position as shown in the figure is obtained. Since the spectral image composed of this foot point becomes a Lissajous figure drawn by the frequency shift signal of the linear FM signal and the vertical sweep signal of the television camera 14, the repetition period of the two signals is slightly shifted from an integral multiple. This creates a fine mesh pattern that uniformly covers the output screen. Therefore, a horizontal scanning direction spatial spectral image of the input image can be displayed on the output screen, and this spectral image becomes a real-time display image according to changes in the input image. The present invention has the above-described configuration, and has the effect that spectrum analysis is possible even for moving images that can be photographed by the television camera 14.
また、テレビカメラおよび撮影装置を固定して使用すれ
ば、対象画像に含まれる空間周波数の絶対値測定も可能
であり、この場合、テレビカメラレンズ系による画像の
拡大、縮小効果を利用すれば、より精度の高い測定も可
能である。さらに、入力すべき映像信号はテレビカメラ
より直接に得た信号に限らず、ビテオテープ等の収録映
像信号も使用できる。Furthermore, if a television camera and photographing device are used in a fixed manner, it is also possible to measure the absolute value of the spatial frequency contained in the target image.In this case, if the image enlargement and reduction effects of the television camera lens system are used, More accurate measurements are also possible. Furthermore, the video signal to be input is not limited to the signal directly obtained from a television camera, but also video signals recorded on a videotape or the like can be used.
第1図は本発明の実施例を示す図、第2図は信号のタイ
ミングチャートを示す図、第3図はスペクトル画像の構
成を示す図、第4図は従来例を示す図、第5図は画像の
双方向水平走査を示す図、第6図は信号のタイミングチ
ャートを示す図。
la,lbは正弦波発振器、2は欠番、3a,3bは広
帯域城増幅器、4はしーザー、5a,5bは超音波光変
調器、6は光検出フィル夕、7は光電変換器、8は映像
信号増幅器、9は映像信号パルス化回路、1川ま同期パ
ルス分離回路、1 1は水平同期時間遅延回路、12は
混合器、13は入力画像、14はテレビカメラ、15は
双方向掃引発振器、16は受像器、17はモニタテレビ
、18は映像信号サンプリング回路、19は自乗圧縮回
路、20は掃引信号発生回路、21は周波数変調発振器
、22は帯域フィル夕、23は出力画像表示器、101
は相関器、102はフーリエ変換光学系、103は線形
FM信号繰返し発生装置、ULMa,ULMbは超音波
光変調器を表わす。第1図第2図
第3図
第4図
第5図
第6図Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 is a diagram showing a signal timing chart, Fig. 3 is a diagram showing the configuration of a spectral image, Fig. 4 is a diagram showing a conventional example, and Fig. 5 6 is a diagram showing bidirectional horizontal scanning of an image, and FIG. 6 is a diagram showing a signal timing chart. la and lb are sine wave oscillators, 2 is a missing number, 3a and 3b are broadband amplifiers, 4 is a Caesar, 5a and 5b are ultrasonic optical modulators, 6 is a photodetection filter, 7 is a photoelectric converter, and 8 is a Video signal amplifier, 9 is a video signal pulsing circuit, 1 is a synchronization pulse separation circuit, 1 is a horizontal synchronization time delay circuit, 12 is a mixer, 13 is an input image, 14 is a television camera, 15 is a bidirectional sweep oscillator , 16 is a television receiver, 17 is a monitor television, 18 is a video signal sampling circuit, 19 is a square compression circuit, 20 is a sweep signal generation circuit, 21 is a frequency modulation oscillator, 22 is a band filter, 23 is an output image display, 101
102 is a correlator, 102 is a Fourier transform optical system, 103 is a linear FM signal repetition generator, and ULMa and ULMb are ultrasonic optical modulators. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6
Claims (1)
せるための画像空間周波数アナライザであつて; 前記
入力画像を水平走査して得られる複合映像信号を出力す
るテレビカメラ14と; 該複合映像信号より水平垂直
パルスを分離し、かつ、各水平走査ごとに得られる前記
映像信号を1走査おきにサンプリングして映像信号の前
後に無信号部分を作る映像信号サンプリング回路18と
; 該無信号部分を有する映像信号を自乗圧縮する自乗
圧縮回路19と; 一定の繰返し周期で線形FM信号を
発生させる線形FM信号から繰返し発生装置103と;
一対の振幅変調可能な正弦波発振器1a,1bと、該
正弦波発振器の出力信号を入力信号とする広帯域増幅器
3a,3bと、該増幅器の出力信号を入力信号とし超音
波伝搬方向が互いに逆向きである一対の超音波光変調器
5a,5bを有するフーリエ変換光学系102と、前記
光学系の光源であるレーザー4と、該光学系の出力光を
検出するフイルタ6と、該出力光を光電変換する光電変
換器7で構成され、無信号部分を有する映像信号と、該
線形FM信号を受領して相互相関信号を出力する相関器
101と; 該線形FM信号繰返し発生装置より出力さ
れる線形FM信号周波数掃引信号、該テレビカメラの垂
直同期掃引信号および該相関器より出力される相互相関
信号を受領して空間周波数スペクトル画像を表示する出
力画像表示器23とを備えたことを特徴とする画像空間
周波数アナライザ。1 An image spatial frequency analyzer for displaying a spatial frequency spectrum image of an input image 13; A television camera 14 that outputs a composite video signal obtained by horizontally scanning the input image; a video signal sampling circuit 18 that separates pulses and samples the video signal obtained for each horizontal scan every other scan to create no-signal portions before and after the video signal; a video signal having the no-signal portion; a square compression circuit 19 that performs square compression; a linear FM signal repetition generator 103 that generates a linear FM signal at a constant repetition period;
A pair of amplitude modulated sine wave oscillators 1a and 1b, broadband amplifiers 3a and 3b whose input signals are the output signals of the sine wave oscillators, and whose ultrasonic propagation directions are opposite to each other and whose input signals are the output signals of the amplifiers. A Fourier transform optical system 102 having a pair of ultrasonic light modulators 5a and 5b, a laser 4 as a light source of the optical system, a filter 6 for detecting the output light of the optical system, and a photoelectric converter for the output light. a correlator 101 that receives the video signal having a no-signal portion and the linear FM signal and outputs a cross-correlation signal; The present invention is characterized by comprising an output image display 23 that receives the FM signal frequency sweep signal, the vertical synchronization sweep signal of the television camera, and the cross-correlation signal output from the correlator and displays a spatial frequency spectrum image. Image spatial frequency analyzer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16657280A JPS6034318B2 (en) | 1980-11-28 | 1980-11-28 | image spatial frequency analyzer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP16657280A JPS6034318B2 (en) | 1980-11-28 | 1980-11-28 | image spatial frequency analyzer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5791087A JPS5791087A (en) | 1982-06-07 |
| JPS6034318B2 true JPS6034318B2 (en) | 1985-08-08 |
Family
ID=15833743
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP16657280A Expired JPS6034318B2 (en) | 1980-11-28 | 1980-11-28 | image spatial frequency analyzer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6034318B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH11101625A (en) * | 1997-09-25 | 1999-04-13 | Mitsubishi Heavy Ind Ltd | Fracture surface analysis method by spatial frequency analysis |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6052821A (en) * | 1983-09-02 | 1985-03-26 | Anritsu Corp | Device for detecting space frequency of image |
| CN106841774B (en) * | 2017-01-24 | 2019-10-25 | 海南大学 | A power system frequency acquisition method and system based on double-layer iteration |
-
1980
- 1980-11-28 JP JP16657280A patent/JPS6034318B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH11101625A (en) * | 1997-09-25 | 1999-04-13 | Mitsubishi Heavy Ind Ltd | Fracture surface analysis method by spatial frequency analysis |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5791087A (en) | 1982-06-07 |
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